2007-04-20 07:25:27 +08:00
|
|
|
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
|
|
|
|
|
|
|
|
:link(lws,http://lammps.sandia.gov)
|
|
|
|
:link(ld,Manual.html)
|
|
|
|
:link(lc,Section_commands.html#comm)
|
|
|
|
|
|
|
|
:line
|
|
|
|
|
|
|
|
compute temp/asphere command :h3
|
|
|
|
|
|
|
|
[Syntax:]
|
|
|
|
|
2008-03-21 08:45:02 +08:00
|
|
|
compute ID group-ID temp/asphere bias-ID :pre
|
2007-04-20 07:25:27 +08:00
|
|
|
|
|
|
|
ID, group-ID are documented in "compute"_compute.html command
|
2008-03-21 08:45:02 +08:00
|
|
|
temp/asphere = style name of this compute command
|
|
|
|
bias-ID = ID of a temperature compute that removes a velocity bias (optional) :ul
|
2007-04-20 07:25:27 +08:00
|
|
|
|
|
|
|
[Examples:]
|
|
|
|
|
|
|
|
compute 1 all temp/asphere
|
2008-03-21 08:45:02 +08:00
|
|
|
compute myTemp mobile temp/asphere tempCOM :pre
|
2007-04-20 07:25:27 +08:00
|
|
|
|
|
|
|
[Description:]
|
|
|
|
|
|
|
|
Define a computation that calculates the temperature of a group of
|
2008-03-18 08:23:39 +08:00
|
|
|
aspherical particles, including a contribution from both their
|
|
|
|
translational and rotational kinetic energy. This differs from the
|
2008-03-19 04:39:07 +08:00
|
|
|
usual "compute temp"_compute_temp.html command, which assumes point
|
|
|
|
particles with only translational kinetic energy.
|
2008-03-18 08:23:39 +08:00
|
|
|
|
|
|
|
For 3d aspherical particles, each has 3, 5, or 6 degrees of freedom (3
|
|
|
|
translational, remainder rotational), depending on whether the
|
|
|
|
particle is spherical, uniaxial, or biaxial. This is determined by
|
|
|
|
the "shape"_shape.html command. Uniaxial means two of its three shape
|
2008-03-19 04:39:07 +08:00
|
|
|
parameters are equal. Biaxial means all 3 shape parameters are
|
|
|
|
different.
|
2008-03-18 08:23:39 +08:00
|
|
|
|
2008-03-19 04:39:07 +08:00
|
|
|
For 2d aspherical particles, each has 3 or 4 degrees of freedom (3
|
|
|
|
translational, remainder rotational), depending on whether the
|
|
|
|
particle is spherical, or biaxial. Biaxial means the x,y shape
|
|
|
|
parameters are unequal.
|
2008-03-18 08:23:39 +08:00
|
|
|
|
|
|
|
IMPORTANT NOTE: These degrees of freedom assume that the interaction
|
|
|
|
potential between degenerate aspherical particles does not impart
|
|
|
|
rotational motion to the extra degrees of freedom. E.g. the "GayBerne
|
|
|
|
pair potential"_pair_gayberne.html does not impart torque to spherical
|
|
|
|
particles, so they do not rotate.
|
|
|
|
|
2009-04-30 00:54:14 +08:00
|
|
|
The translational kinetic energy is computed the same as is described
|
|
|
|
by the "compute temp"_compute_temp.html command. The rotational
|
|
|
|
kinetic energy is computed as 1/2 I w^2, where I is the inertia tensor
|
|
|
|
for the aspherical particle and w is its angular velocity, which is
|
|
|
|
computed from its angular momentum.
|
2008-03-19 04:39:07 +08:00
|
|
|
|
2008-03-19 05:02:30 +08:00
|
|
|
IMPORTANT NOTE: For "2d models"_dimension.html, particles are treated
|
2008-03-19 04:39:07 +08:00
|
|
|
as ellipsoids, not ellipses, meaning their moments of inertia will be
|
|
|
|
the same as in 3d.
|
2008-03-18 08:23:39 +08:00
|
|
|
|
|
|
|
A 6-component kinetic energy tensor is also calculated by this
|
|
|
|
compute. The formula for the components of the tensor is the same as
|
|
|
|
the above formula, except that v^2 and w^2 are replaced by vx*vy and
|
|
|
|
wx*wy for the xy component, and the appropriate elements of the
|
|
|
|
inertia tensor are used.
|
|
|
|
|
|
|
|
The number of atoms contributing to the temperature is assumed to be
|
|
|
|
constant for the duration of the run; use the {dynamic} option of the
|
|
|
|
"compute_modify"_compute_modify.html command if this is not the case.
|
|
|
|
|
2008-03-21 08:45:02 +08:00
|
|
|
If a {bias-ID} is specified it must be the ID of a temperature compute
|
|
|
|
that removes a "bias" velocity from each atom. This allows compute
|
|
|
|
temp/sphere to compute its thermal temperature after the translational
|
|
|
|
kinetic energy components have been altered in a prescribed way,
|
|
|
|
e.g. to remove a velocity profile. Thermostats that use this compute
|
|
|
|
will work with this bias term. See the doc pages for individual
|
|
|
|
computes that calculate a temperature and the doc pages for fixes that
|
|
|
|
perform thermostatting for more details.
|
|
|
|
|
2008-03-18 08:23:39 +08:00
|
|
|
This compute subtracts out translational degrees-of-freedom due to
|
|
|
|
fixes that constrain molecular motion, such as "fix
|
|
|
|
shake"_fix_shake.html and "fix rigid"_fix_rigid.html. This means the
|
|
|
|
temperature of groups of atoms that include these constraints will be
|
|
|
|
computed correctly. If needed, the subtracted degrees-of-freedom can
|
|
|
|
be altered using the {extra} option of the
|
|
|
|
"compute_modify"_compute_modify.html command.
|
2007-04-20 07:25:27 +08:00
|
|
|
|
2008-04-07 23:58:34 +08:00
|
|
|
See "this howto section"_Section_howto.html#4_16 of the manual for a
|
|
|
|
discussion of different ways to compute temperature and perform
|
|
|
|
thermostatting.
|
|
|
|
|
2008-01-03 03:25:15 +08:00
|
|
|
[Output info:]
|
|
|
|
|
|
|
|
The scalar value calculated by this compute is "intensive", meaning it
|
|
|
|
is independent of the number of atoms in the simulation. The vector
|
|
|
|
values are "extensive", meaning they scale with the number of atoms in
|
|
|
|
the simulation.
|
|
|
|
|
2007-04-20 07:25:27 +08:00
|
|
|
[Restrictions:]
|
|
|
|
|
2008-03-18 08:23:39 +08:00
|
|
|
This compute requires that particles be represented as extended
|
|
|
|
ellipsoids and not point particles. This means they will have an
|
|
|
|
angular momentum and a shape which is determined by the
|
|
|
|
"shape"_shape.html command.
|
2007-04-20 07:25:27 +08:00
|
|
|
|
|
|
|
[Related commands:]
|
|
|
|
|
|
|
|
"compute temp"_compute_temp.html
|
|
|
|
|
|
|
|
[Default:] none
|